Eliminate the lower component to get (E2−m2c4)φ=c2(σ⋅Π)2φ. Since [Πx,Πy]=ieℏB/c, the Pauli identity gives (σ⋅Π)2=Π2−eℏBσ3/c. Substitute the three momenta and rearrange:The spin-field sign follows from the charge convention and commutator, not an independent assignment.
[dy2d2−ℏ2c2(pxc+eBy)2+ℏ2c2E2−m2c4−ℏ2pz2+ℏceBσ3]φ=0.
Ancestors (12)
- 2
- 3
- S18
- 2017
- Past exam of the short options paper shared by Prelims and Parts A and B of the physics course of the University of Oxford
- Short options paper shared by Prelims and Parts A and B of the physics course of the University of Oxford
- Physics course of the University of Oxford
- Undergraduate course of the University of Oxford
- Course of the University of Oxford
- University of Oxford
- List of universities
- Home
Discussion (0)
New discussionThere are no discussions about this article yet.
Articles by others on the same topic (0)
There are currently no matching articles.